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At what speed is the momentum of a particle three times as great as the result obtained from the nonrelativistic expression \(m v ?\)

Short Answer

Expert verified
At \( v = \frac{2\sqrt{2}}{3} c \), the momentum is three times the classical value.

Step by step solution

01

Understanding Nonrelativistic Momentum

In classical physics, the momentum of a particle is given by the formula \( p = m v \), where \( m \) is the mass of the particle and \( v \) is the velocity. We need to find when the relativistic momentum is three times this value.
02

Understanding Relativistic Momentum

Relativistic momentum takes into account relativistic effects at high velocities and is given by the formula \( p = \frac{m v}{\sqrt{1-(v^2/c^2)}} \), where \( c \) is the speed of light. We set this equal to \( 3m v \) to represent three times the classical momentum.
03

Set Up the Equation

To find the velocity where the relativistic momentum is three times the nonrelativistic momentum, set the equation: \[ \frac{m v}{\sqrt{1-(v^2/c^2)}} = 3 m v \]. Simplifying, the mass and velocity terms cancel, leaving \[ \frac{1}{\sqrt{1-(v^2/c^2)}} = 3 \].
04

Solve for Velocity

Square both sides of the equation \( \frac{1}{\sqrt{1-(v^2/c^2)}} = 3 \) to get \( 1-{v^2/c^2} = \frac{1}{9} \). Rearrange to solve for \( v^2: \quad v^2/c^2 = 8/9 \). Multiply through by \( c^2 \) to find \( v^2 = 8c^2/9 \). Taking the square root of both sides gives \( v = \frac{\sqrt{8}}{3} c \).
05

Final Result

The velocity at which the relativistic momentum of the particle is three times the nonrelativistic momentum is \( v = \frac{2\sqrt{2}}{3} c \).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Nonrelativistic Momentum
In classical physics, nonrelativistic momentum is defined by the simple formula \( p = m v \). Here, \( m \) represents the mass of the particle and \( v \) is the velocity of the particle.
This concept is based on Newtonian mechanics, which assumes that particles move at speeds much lower than the speed of light. At these speeds, relativistic effects are negligible and the formula provides an accurate measure of momentum.
Nonrelativistic momentum is straightforward and is often used in everyday physics problems where speeds are not extremely high. This simplicity, however, fails at speeds approaching the speed of light, where relativistic effects must be considered.
Momentum in Physics
Momentum is a fundamental concept in physics that describes the quantity of motion of a moving body. It is a vector, meaning it has both magnitude and direction. Momentum is conserved in isolated systems, making it a crucial component in analyzing collisions and interactions.
Understanding momentum helps explain various phenomena, from everyday objects in motion to the behavior of celestial bodies. In different contexts, momentum will take on different forms. For example, in purely classical situations, we use nonrelativistic momentum, while in high-speed or high-energy scenarios, relativistic momentum is employed.
Thus, momentum bridges classical physics with modern physics, adapting its expression depending on the speed and nature of the particles involved.
Velocity of Particles
Velocity is the rate of change of an object's position with respect to time and is a key variable in calculating both nonrelativistic and relativistic momentum. It is different from speed, which is a scalar quantity, having no direction.
The dynamics of particle velocity play a central role in physics, as it influences the overall momentum and kinetic energy of the particles involved. As particles approach the speed of light, classical calculations of velocity begin to fail and relativistic physics takes precedence.
This change is due to the relativistic effects that arise, which adjust the momentum formula to account for the increase in mass that occurs at these high velocities.
Relativistic Effects
As objects move at velocities close to the speed of light, they experience relativistic effects. These effects alter the fundamental calculations of physics, including mass, energy, and momentum.
According to Einstein's theory of relativity, mass effectively increases with an object's velocity, necessitating the use of the relativistic momentum formula: \( p = \frac{m v}{\sqrt{1-(v^2/c^2)}} \). This formula corrects for the significant changes in momentum that occur at high speeds, ensuring accurate predictions in particle physics and cosmological studies.
These modifications underscore the importance of considering relativistic effects in any high-speed scenarios, where classical physics may not apply.
Speed of Light
The speed of light, denoted \( c \), is approximately \( 3 \times 10^8 \) meters per second and is a fundamental constant in the universe. It acts as the ultimate speed limit for any object with mass.
The significance of the speed of light stems from its role in the theory of relativity, where it acts as a critical threshold for observing relativistic effects. As an object approaches this speed, time slows and length contracts, drastically altering its physical characteristics and measurements.
Understanding the speed of light is crucial for fields such as astrophysics and quantum mechanics, where high velocities are commonplace and relativity must be accounted for in all analyses.

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Most popular questions from this chapter

Space travel? Travel to the stars requires hundreds or thousands of years, even at the speed of light. Some people have suggested that we can get around this difficulty by accelerating the rocket (and its astronauts) to very high speeds so that they will age less due to time dilation. The fly in this ointment is that it takes a great deal of energy to do this. Suppose you want to go to the immense red giant Betelgeuse, which is about 500 light-years away. You plan to travel at constant speed in a \(1000 \mathrm{~kg}\) rocket ship (a little over a ton), which, in reality, is far too small for this purpose. In each case that follows, calculate the time for the trip, as measured by people on earth and by astronauts in the rocket ship, the energy needed in joules, and the energy needed as a percent of U.S. yearly use (which is \(1.0 \times 10^{20} \mathrm{~J}\) ). For comparison, arrange your results in a table showing \(v_{\text {rocket }}, t_{\text {earth }}, t_{\text {rocket }}, E(\) in \(\mathbf{J}),\) and \(E\) (as \(\%\) of U.S. use). The rocket ship's speed is (a) \(0.50 c,\) (b) \(0.99 c\), and (c) \(0.9999 c\). On the basis of your results, does it seem likely that any government will invest in such high- speed space travel any time soon?

An electron is acted upon by a force of \(5.00 \times 10^{-15} \mathrm{~N}\) due to an electric field. Find the acceleration this force produces in each case: (a) The electron's speed is \(1.00 \mathrm{~km} / \mathrm{s}\). (b) The electron's speed is \(2.50 \times 10^{8} \mathrm{~m} / \mathrm{s}\) and the force is parallel to the velocity.

A space probe is sent to the vicinity of the star Capella, which is 42.2 light-years from the earth. The probe travels with a speed of \(0.9910 c\) relative to the earth. An astronaut recruit on board is 19 years old when the probe leaves the earth. What is her biological age when the probe reaches Capella, as measured by (a) the astronaut and (b) someone on earth?

A spacecraft is moving at a speed of \(0.800 c\) relative to the earth. What is the ratio of the length of the spacecraft, as viewed through a telescope on earth, to its length when measured after landing on earth? (Assume that the spacecraft is moving at a right angle to the line of observation.

A cube of metal with sides of length \(a\) sits at rest in the laboratory with one edge parallel to the \(x\) axis. Therefore, in the laboratory frame, its volume is \(a^{3}\). A rocket ship flies past the laboratory parallel to the \(x\) axis with a velocity \(v .\) As measured by an observer in the rocket, determine (a) the length of the edges of the cube that are perpendicular to the \(x\) axis, (b) the length of the cube edges that are parallel to the \(x\) axis, and (c) the volume of the metal cube.

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